Type II embeddings for d = 6 Einstein-Maxwell gauged supergravity

A bstract Bi-spinor and G-structure methods are used to classify the possible consistent truncations of type II supergravity to d = 6 Einstein-Maxwell (gauged) supergravity, and its consistent sub-sectors. In the absence of R-symmetry gauging and a tensor multiplet we establish that every supersymmetric Mink 6 solution defines an embedding of the d = 6 theory. Adding a tensor multiplet places restrictions on these embeddings, but embeddings still exist. In the presence of R-symmetry gauging the internal spaces of the embeddings are neither related to Mink 6 or AdS 6 . Under the assumption that the internal space contains a single U(1) isometry housing the d = 6 gauge field we classify the possible embedding manifolds. We find two classes of embedding for the entire theory, one of which is governed by a Toda-like equation and contains at least one prototype bounded embedding, albeit containing likely un-physical singularities. In the absence of a tensor multiple the classes of embeddings become more permissive, though the PDEs governing them become more complicated in general.

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Publication Details

Journal
Journal of High Energy Physics
Published
2026-09-04
DOI
https://doi.org/10.1007/jhep09(2026)071
Primary Topic
Black Holes and Theoretical Physics
Type
article
Field-Weighted Citation Impact
0.00

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article

Type II embeddings for d = 6 Einstein-Maxwell gauged supergravity

Journal of High Energy Physics
Black Holes and Theoretical Physics
article

Type II embeddings for d = 6 Einstein-Maxwell gauged supergravity

article en

Abstract

A bstract Bi-spinor and G-structure methods are used to classify the possible consistent truncations of type II supergravity to d = 6 Einstein-Maxwell (gauged) supergravity, and its consistent sub-sectors. In the absence of R-symmetry gauging and a tensor multiplet we establish that every supersymmetric Mink 6 solution defines an embedding of the d = 6 theory. Adding a tensor multiplet places restrictions on these embeddings, but embeddings still exist. In the presence of R-symmetry gauging the internal spaces of the embeddings are neither related to Mink 6 or AdS 6 . Under the assumption that the internal space contains a single U(1) isometry housing the d = 6 gauge field we classify the possible embedding manifolds. We find two classes of embedding for the entire theory, one of which is governed by a Toda-like equation and contains at least one prototype bounded embedding, albeit containing likely un-physical singularities. In the absence of a tensor multiple the classes of embeddings become more permissive, though the PDEs governing them become more complicated in general.

Journal of High Energy PhysicsVol. 2026(9)
Universidad de Oviedo (ES)
Simons Foundation, Ministerio de Ciencia, Innovación y Universidades
Openalex Percentile: Top 94%
Black Holes and Theoretical Physics
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